Enhancement or quenching effect of metallic nanodimer on spontaneous emission
The plasmonic effects of a metallic (Au or Ag) nanodimer on the excitation and emission of a single emitter placed within the gap of the nanodimer are studied to identify its overall performance (enhancement or quenching) for the spontaneous emission. The process of a spontaneous emission is divided...
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Veröffentlicht in: | Journal of quantitative spectroscopy & radiative transfer 2010-02, Vol.111 (3), p.454-465 |
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creator | Liaw, Jiunn-Woei Chen, Chi-San Chen, Jeng-Hong |
description | The plasmonic effects of a metallic (Au or Ag) nanodimer on the excitation and emission of a single emitter placed within the gap of the nanodimer are studied to identify its overall performance (enhancement or quenching) for the spontaneous emission. The process of a spontaneous emission is divided into two stages for analysis: the excitation and the subsequent emission stages. For the excitation stage, the amplification of the local electric field around the gap region is studied to show the converging-lens effect of the nanodimer for focusing an incident light. For the emission stage, the apparent quantum yield of an electric dipole (the excited emitter) in the presence of the nanodimer is studied in terms of its radiative and nonradiative decay rates. Both models are simulated by the multiple multi-pole methods for solving Maxwell's equations. The results indicate that the overall enhancement factor of a metallic nanodimer on the spontaneous emission depends not only on its dimension (radius and gap) but also on the absorption and emission spectra of the emitter. Moreover, there is an optimal dimension (radius and gap) of a nanodimer for obtaining the maximum enhancement to a specific spontaneous emission. In addition, the observed emission spectrum of the emitter can be modified by the nearby nanodimer (a low-pass filter), and its lifetime can be reduced by two or three orders of magnitude due to the energy transfer between them. |
doi_str_mv | 10.1016/j.jqsrt.2009.09.009 |
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The process of a spontaneous emission is divided into two stages for analysis: the excitation and the subsequent emission stages. For the excitation stage, the amplification of the local electric field around the gap region is studied to show the converging-lens effect of the nanodimer for focusing an incident light. For the emission stage, the apparent quantum yield of an electric dipole (the excited emitter) in the presence of the nanodimer is studied in terms of its radiative and nonradiative decay rates. Both models are simulated by the multiple multi-pole methods for solving Maxwell's equations. The results indicate that the overall enhancement factor of a metallic nanodimer on the spontaneous emission depends not only on its dimension (radius and gap) but also on the absorption and emission spectra of the emitter. Moreover, there is an optimal dimension (radius and gap) of a nanodimer for obtaining the maximum enhancement to a specific spontaneous emission. In addition, the observed emission spectrum of the emitter can be modified by the nearby nanodimer (a low-pass filter), and its lifetime can be reduced by two or three orders of magnitude due to the energy transfer between them.</description><identifier>ISSN: 0022-4073</identifier><identifier>EISSN: 1879-1352</identifier><identifier>DOI: 10.1016/j.jqsrt.2009.09.009</identifier><language>eng</language><publisher>Elsevier Ltd</publisher><subject>Apparent quantum yield ; Excitation rate ; Lifetime ; MMP ; Nanodimer ; Nonradiative decay rate ; Radiative decay rate ; Spontaneous emission</subject><ispartof>Journal of quantitative spectroscopy & radiative transfer, 2010-02, Vol.111 (3), p.454-465</ispartof><rights>2009 Elsevier Ltd</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c334t-9e2ee1b53fe2453cad67ffa5324e7fb0c8d5305892b8425df2db2d32bcdc6efa3</citedby><cites>FETCH-LOGICAL-c334t-9e2ee1b53fe2453cad67ffa5324e7fb0c8d5305892b8425df2db2d32bcdc6efa3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://dx.doi.org/10.1016/j.jqsrt.2009.09.009$$EHTML$$P50$$Gelsevier$$H</linktohtml><link.rule.ids>314,778,782,3539,27907,27908,45978</link.rule.ids></links><search><creatorcontrib>Liaw, Jiunn-Woei</creatorcontrib><creatorcontrib>Chen, Chi-San</creatorcontrib><creatorcontrib>Chen, Jeng-Hong</creatorcontrib><title>Enhancement or quenching effect of metallic nanodimer on spontaneous emission</title><title>Journal of quantitative spectroscopy & radiative transfer</title><description>The plasmonic effects of a metallic (Au or Ag) nanodimer on the excitation and emission of a single emitter placed within the gap of the nanodimer are studied to identify its overall performance (enhancement or quenching) for the spontaneous emission. The process of a spontaneous emission is divided into two stages for analysis: the excitation and the subsequent emission stages. For the excitation stage, the amplification of the local electric field around the gap region is studied to show the converging-lens effect of the nanodimer for focusing an incident light. For the emission stage, the apparent quantum yield of an electric dipole (the excited emitter) in the presence of the nanodimer is studied in terms of its radiative and nonradiative decay rates. Both models are simulated by the multiple multi-pole methods for solving Maxwell's equations. The results indicate that the overall enhancement factor of a metallic nanodimer on the spontaneous emission depends not only on its dimension (radius and gap) but also on the absorption and emission spectra of the emitter. Moreover, there is an optimal dimension (radius and gap) of a nanodimer for obtaining the maximum enhancement to a specific spontaneous emission. In addition, the observed emission spectrum of the emitter can be modified by the nearby nanodimer (a low-pass filter), and its lifetime can be reduced by two or three orders of magnitude due to the energy transfer between them.</description><subject>Apparent quantum yield</subject><subject>Excitation rate</subject><subject>Lifetime</subject><subject>MMP</subject><subject>Nanodimer</subject><subject>Nonradiative decay rate</subject><subject>Radiative decay rate</subject><subject>Spontaneous emission</subject><issn>0022-4073</issn><issn>1879-1352</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2010</creationdate><recordtype>article</recordtype><recordid>eNp9kEtLxDAUhYMoOD5-gZus3LXm0fSxcCHD-IARN7oOaXLjpLTJTNIR_Pe21rVw4MLlnMu5H0I3lOSU0PKuy7tDimPOCGnyWaQ5QStaV01GuWCnaEUIY1lBKn6OLlLqCCGc03KFXjd-p7yGAfyIQ8SHI3i9c_4Tg7Wgp53FA4yq753GXvlg3AARB4_TPvhReQjHhGFwKbngr9CZVX2C6795iT4eN-_r52z79vSyfthmmvNizBpgALQV3AIrBNfKlJW1SnBWQGVbomsjOBF1w9q6YMJYZlpmOGu10SVYxS_R7XJ3H8PUOI1yKqCh75c-kpdFLWrGJiNfjDqGlCJYuY9uUPFbUiJndLKTv-jkjE7OIs2Uul9SMP3w5SDKpN3EBYyLExNpgvs3_wM0K3sE</recordid><startdate>20100201</startdate><enddate>20100201</enddate><creator>Liaw, Jiunn-Woei</creator><creator>Chen, Chi-San</creator><creator>Chen, Jeng-Hong</creator><general>Elsevier Ltd</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7SR</scope><scope>7U5</scope><scope>8BQ</scope><scope>8FD</scope><scope>JG9</scope><scope>L7M</scope></search><sort><creationdate>20100201</creationdate><title>Enhancement or quenching effect of metallic nanodimer on spontaneous emission</title><author>Liaw, Jiunn-Woei ; Chen, Chi-San ; Chen, Jeng-Hong</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c334t-9e2ee1b53fe2453cad67ffa5324e7fb0c8d5305892b8425df2db2d32bcdc6efa3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2010</creationdate><topic>Apparent quantum yield</topic><topic>Excitation rate</topic><topic>Lifetime</topic><topic>MMP</topic><topic>Nanodimer</topic><topic>Nonradiative decay rate</topic><topic>Radiative decay rate</topic><topic>Spontaneous emission</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Liaw, Jiunn-Woei</creatorcontrib><creatorcontrib>Chen, Chi-San</creatorcontrib><creatorcontrib>Chen, Jeng-Hong</creatorcontrib><collection>CrossRef</collection><collection>Engineered Materials Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>METADEX</collection><collection>Technology Research Database</collection><collection>Materials Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Journal of quantitative spectroscopy & radiative transfer</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Liaw, Jiunn-Woei</au><au>Chen, Chi-San</au><au>Chen, Jeng-Hong</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Enhancement or quenching effect of metallic nanodimer on spontaneous emission</atitle><jtitle>Journal of quantitative spectroscopy & radiative transfer</jtitle><date>2010-02-01</date><risdate>2010</risdate><volume>111</volume><issue>3</issue><spage>454</spage><epage>465</epage><pages>454-465</pages><issn>0022-4073</issn><eissn>1879-1352</eissn><abstract>The plasmonic effects of a metallic (Au or Ag) nanodimer on the excitation and emission of a single emitter placed within the gap of the nanodimer are studied to identify its overall performance (enhancement or quenching) for the spontaneous emission. The process of a spontaneous emission is divided into two stages for analysis: the excitation and the subsequent emission stages. For the excitation stage, the amplification of the local electric field around the gap region is studied to show the converging-lens effect of the nanodimer for focusing an incident light. For the emission stage, the apparent quantum yield of an electric dipole (the excited emitter) in the presence of the nanodimer is studied in terms of its radiative and nonradiative decay rates. Both models are simulated by the multiple multi-pole methods for solving Maxwell's equations. The results indicate that the overall enhancement factor of a metallic nanodimer on the spontaneous emission depends not only on its dimension (radius and gap) but also on the absorption and emission spectra of the emitter. Moreover, there is an optimal dimension (radius and gap) of a nanodimer for obtaining the maximum enhancement to a specific spontaneous emission. In addition, the observed emission spectrum of the emitter can be modified by the nearby nanodimer (a low-pass filter), and its lifetime can be reduced by two or three orders of magnitude due to the energy transfer between them.</abstract><pub>Elsevier Ltd</pub><doi>10.1016/j.jqsrt.2009.09.009</doi><tpages>12</tpages></addata></record> |
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subjects | Apparent quantum yield Excitation rate Lifetime MMP Nanodimer Nonradiative decay rate Radiative decay rate Spontaneous emission |
title | Enhancement or quenching effect of metallic nanodimer on spontaneous emission |
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